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Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

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Two-dimensional Cascades 85<br />

FIG. 3.25. Pr<strong>of</strong>ile loss coefficients <strong>of</strong> turbine nozzle <strong>and</strong> impulse blades at zero<br />

incidence (t/l = 20%; Re = 2 ¥ 10 5 ; M < 0.6) (adapted from Ainley <strong>and</strong> Mathieson 1951).<br />

where all the values <strong>of</strong> Yp are taken at the same space–chord ratio <strong>and</strong> flow outlet<br />

angle. If rotor blades are being considered, put 3b2 for a1 <strong>and</strong> b3 for a2. Equation<br />

(3.46) includes a correction for the effect <strong>of</strong> thickness–chord ratio <strong>and</strong> is valid in<br />

the range 0.15 t/l 0.25. If the actual blade has a t/l greater or less than the<br />

limits quoted, Ainley recommends that the loss should be taken as equal to a blade<br />

having t/l either 0.25 or 0.15. By substituting a1 = a2 <strong>and</strong> t/l = 0.2 in eqn. (3.46),<br />

the zero incidence loss coefficient for the impulse blades Yp(a1=a2) given in Figure<br />

3.25 is recovered. Similarly, with a 1 = 0 at t/l = 0.2 in eqn. (3.46) gives Yp(a1= 0) <strong>of</strong> Figure<br />

3.25.<br />

A feature <strong>of</strong> the losses given in Figure 3.25 is that, compared with the impulse<br />

blades, the nozzle blades have a much lower loss coefficient. This trend confirms<br />

the results shown in Figure 3.14, that flow in which the mean pressure is falling

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